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and the first term for
j
◦
S
is
ζ
−b
e
−
2
πiaτ/d
=
ζ
−b
(
e
−
2
πiτ/N
)
a
2
.
=
a
2
. Therefore, these terms represent
different powers of
e
2
πiτ/N
, so they cannot cancel each other. One of them
must be the first term of the expansion of
j − j ◦ S
, which therefore has
coecient 1 or
−ζ
b
. In particular, for each factor
j − j ◦ S
, the coecient of
the first term of the expansion is a root of unity. The coecient of the first
term of the expansion of
H
N
(
j
) is the product of these roots of unity, hence
a root of unity. Also, since the terms don't cancel each other, the first term
of each factor contains a negative power of
e
2
πiτ/N
. Therefore, the first term
of the expansion
H
N
(
j
) is a negative power of
q
,so
H
N
(
X
)isnonconstant.
Suppose
H
N
(
X
)=
uX
+ lower terms. We know that
u
Since
N
is not a perfect square,
N
∈
Z
. Since the
Laurent series for
j
starts with 1
/q
,
H
N
(
j
)=
uq
−
+higher terms
.
We have shown that
u
is a root of unity. Since it is an integer,
u
=
±
1. This
completes the proof of (2).
The
modular polynomial
Φ
N
(
X, Y
) has rather large coe
cients.
For
example,
X
2
Y
2
+
X
3
+
Y
3
+2
4
Φ
2
(
X, Y
)=
−
·
3
·
31
XY
(
X
+
Y
)
+3
4
5
3
2
4
3
4
5
3
(
X
2
+
Y
2
)
·
·
4027
XY
−
·
·
+2
8
·
3
7
·
5
6
(
X
+
Y
)
−
2
12
·
3
9
·
5
9
,
and
−
1069956
X
3
Y
+ 36864000
X
3
+2232
X
2
Y
3
+ 2587918086
X
2
Y
2
+ 8900222976000
X
2
Y
+452984832000000
X
2
=
X
4
− X
3
Y
3
+ 2232
X
3
Y
2
Φ
3
(
X, Y
)
1069956
XY
3
+ 8900222976000
XY
2
−
770845966336000000
XY
+ 1855425871872000000000
X
+
Y
4
+36864000
Y
3
+ 452984832000000
Y
2
+ 1855425871872000000000
Y
−
For Φ
N
for higher
N
, see [50], [53], [54].
We can now prove Theorem 10.9. Let
R
be an order in an imaginary
quadratic field and let
L
be a lattice with
RL
⊆
L
. By multiplying
L
by a
suitable factor, we may assume that
L
=
Z
+
Z
τ
with
τ ∈H
. T
he o
rder
R
is o
f fin
ite index in
O
K
for some imaginary quadratic
fiel
d
K
=
Q
(
√
−d
). Since
√
−d ∈O
K
, there is a nonzero integer
n
such that
n
√
−
R
. Therefore,
n
√
−
d
∈
L
,so
n
√
−d · τ
=
tτ
+
u,
dL
⊆
n
√
−d ·
1=
vτ
+
w
(10.3)
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